Abstract

We measure the ultrafast recombination of photoexcited quasiparticles (holon-doublon pairs) in the one dimensional Mott insulator ET-F(2)TCNQ as a function of external pressure, which is used to tune the electronic structure. At each pressure value, we first fit the static optical properties and extract the electronic bandwidth t and the intersite correlation energy V. We then measure the recombination times as a function of pressure, and we correlate them with the corresponding microscopic parameters. We find that the recombination times scale differently than for metals and semiconductors. A fit to our data based on the time-dependent extended Hubbard Hamiltonian suggests that the competition between local recombination and delocalization of the Mott-Hubbard exciton dictates the efficiency of the recombination.

Highlights

  • We measure the ultrafast recombination of photoexcited quasiparticles in the one dimensional Mott insulator ET–F2TCNQ as a function of external pressure, which is used to tune the electronic structure

  • In the case of metals, the dynamics are well captured by the two-temperature model [1,2], which considers the energy stored in the optically excited nonequilibrium electron distribution as flowing into the lattice at a rate determined by the electronphonon coupling strength and by the electronic and lattice heat capacities

  • As the relaxation of hot electrons accelerates with smaller electronic specific heat, and because cev is proportional to the density of states at the Fermi level [3], for metals relaxation should accelerate linearly with the reciprocal of the bandwidth τ ∝ 1=t

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Summary

Introduction

We measure the ultrafast recombination of photoexcited quasiparticles (holon-doublon pairs) in the one dimensional Mott insulator ET–F2TCNQ as a function of external pressure, which is used to tune the electronic structure. We first fit the static optical properties and extract the electronic bandwidth t and the intersite correlation energy V.

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